It is first argued that to permit any flow development of the type con
sidered, the usual Bingham model must be relaxed to permit some deform
ation of the unyielded material. This is done here by adopting a two-v
iscosity model in which the unyielded material is modelled as a Newton
ian liquid of large viscosity. The problem is then solved in the case
of small viscosity ratio and large yield stress. In this way the const
itutive model is close to the Bingham model, and the yielded zones occ
upy thin boundary layers next to the channel walls. The resulting prob
lem is non-linear but the main difficulties concerning the location of
the yield surfaces are removed.